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C-Mod Transport Program. PAC 2007 Presented by Martin Greenwald MIT – Plasma Science & Fusion Center 1/24/2007. Introduction – Programmatic Focus. Upgrades Offer Opportunities Aligned With Transport Interests LHCD – efficient, high-power, off-axis current drive
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C-Mod Transport Program PAC 2007 Presented by Martin Greenwald MIT – Plasma Science & Fusion Center 1/24/2007
Introduction – Programmatic Focus • Upgrades Offer Opportunities Aligned With Transport Interests • LHCD – efficient, high-power, off-axis current drive • Direct manipulation of magnetic shear • Cryopump extend range of collisionality • Improvements in profile and fluctuation diagnostics • Transport is a broad topic – where do we focus (in general)? • Where C-Mod has unique capabilities, runs in unique regimes or observes unique or unusual phenomena. • tei<<tE, Ti = Te , n* range, no core particle or momentum sources • Where we can make important comparisons with other devices especially in support of ITER
Where Do We Focus In Particular?Transport Themes For 2007 Campaign • Tests of standard models for ion transport: • Effects of magnetic shear (exploitation of LHCD) • Effects of collisionality (exploitation of cryopump) • Investigations into other transport channels including • Momentum – predict rotation with low torque, low r* ? • Electron energy - no ignorable energy channel • Particle and impurities – density profiles with no core source? • H-mode physics • Thresholds - especially role of edge flows, topology • Pedestal structure – width and height, rotation and Ti profiles • Pedestal relaxation – especially small/no ELM regimes • ITB physics • Turbulence suppression mechanism (not ExB) • Control of barrier location and strength Ti Fusion Performance – underlying physics of ITER baseline scenario – underlying physics of advanced scenarios
Transport Is An Important Element For Program Thrusts and Many Of Our Topical Groups • Tests of standard models for ion transport • Effects of magnetic shear (edge, baseline & advanced scenarios) • Effects of collisionality (edge) • Investigations into other transport channels including • Momentum (baseline scenarios, MHD and edge) • Electron energy (advanced scenarios) • Particle (baseline & advanced scenarios and edge) • H-modes • Thresholds (baseline scenarios) • Pedestal studies (baseline scenarios) • Pedestal relaxation (baseline scenarios & MHD) • ITBs (advanced scenarios)
Comparisons With Theory And Modeling Form A Critical Part Of The Program • Prediction and control are the ultimate goals of transport studies. • Experiments and theory have progressed to the point where meaningful, quantitative tests are being made. • Theory plays critical role in motivation and design of most of our transport experiments - synthetic diagnostic development • Validation of codes is an emerging theme in the transport community • We have close collaborations with theory and modeling groups at MIT and elsewhere – these will continue. • C-Mod contributions for upgraded local Beowulf cluster (will allow nonlinear gk runs locally)
Exploitation of LHCD: Steady-state Control Of Magnetic Shear • With Te ~ Ti , g > wExB , ZEFF << Z, R/Ln < R/LT; magnetic shear (Ŝ) is one of the few parameters predicted by drift-wave simulations to determine R/LT. • We can exploit LHCD to allow direct manipulation of shear. • High Priority Experiment: Test ITG models by evaluating change in R/LT and fluctuations as we modify Ŝ (lowish density L-modes with current LH power levels). • Note additional work on effects of magnetic shear in pedestal and edge studies From linear ITG calculations – IFS-PPPL model Kotchenreuther et al, 1995
These Experiments Underpin ITB, Hybrid-Mode Research Area • Goal: Profile control via transport control • At weak or reversed shear, instability growth rates are predicted to be much lower (also - suppression of sawteeth with q > 1) • With Ŝ near or below 1 (and weak ExB flow shear!), can we create and maintain ITBs with strong central heating? • Can we produce simultaneous barriers in electron and ion transport channels? • Can we increase core gradients (and bootstrap current)? • Control barrier strength and position? • What are effects of rational q surfaces? • For AT we need to understand the underlying transport physics
Plasma Profiles Drift Waves Zonal Flows Collisional Damping Collisionless Damping Impact Of Collisionality On Transport Has Become An Important Issue • Physics Issues – nonlinear regulation of turbulence • ITG - effects through change in electron dynamics • Reduction of ITG instability drive predicted to be more important than zonal flow damping? • TEM – Drives and dissipation? Effects on particle transport and density profile? • Practical Issue: density profile
Angioni PRL 2003 C-Mod Test Collisionality Effects on Particle Transport/Density Profile With No Particle Source • ITER Interest – better fusion performance with moderate density peaking • Results from ASDEX, JET at low n* • We’ve begun work on this (in a high-triangularity shape) • High Priority Experiment: Exploit cryopump to broaden experimental base, scan n*, d, q95 (ITPA CDB-9) • Pedestal studies carried out at same time Addition of C-Mod data suggest that neff is appropriate scaling variable rather than n/nG (These are strongly correlated, especially on any given machine) – Good news for ITER
C-Mod to match (2007) DIII-D to match (2007) Momentum Transport and Self-Generated Rotation • Rotation is critical for stabilization of turbulence and MHD • But we’re moving toward low torque, low r* regimes (ITER) • What is the origin and scaling of self-generated flows? • What is the role of boundary flows, neutrals? • Is there a steep rotation pedestal? • If so, how is momentum transported in that region? (deGrassie, Rice) Initial C-Mod/DIII-D dimensionless identity experiments have demonstrated match
Momentum Transport Research Plans Major diagnostic initiative HIREX III + NeSox + CXRS • High Priority Expt: Multi-machine studies w/ITPA (in baseline scenarios area) • High Priority Expt: Dimensionless scaling experiments w/DIII-D (in baseline scenarios area) • High Priority Expt: Magnetic braking (in baseline scenarios area) • High Priority Expt: Pedestal rotation profiles and transport + SOL-edge-core coupling • Compare with theory, gk simulations (Ince-Cushman, Rice, Bitter, Hill) New high-resolution x-ray spectrometer (HIREX III) with increased radial coverage, resolution, time response (part of MIT/PPPL collaboration)
kq ~ 50 cm-1 kq ~ 30 cm-1 Electron Energy Transport • High Priority Expt: PCI upgrades allow localized measurements of fluctuations at k up to 50 cm-1 • This should be adequate for comparison with coupled ITG-TEM-ETG simulations (Waltz & Candy) • Test in electron dominated plasmas • High Priority Expt: Investigate electron transport with localized transient perturbations from LHH. (Lin)
Particle and Impurity Transport • ITER • What will density profiles be? Impurity content? Fueling requirements? • Collisionality dependence (Experiment as noted earlier) ? • Relative importance of TEM and ITG in particle transport? • Gyrokinetic studies with gs2, gyro (TEM identified in ITB) • LHCD should enable extension of Tore Supra experiments with no core source or Ware pinch (Use VL = 0 LHCD experiments) • High Priority Expt on poloidal asymmetries in impurity particle densities • We’re rebuilding laser blow-off equipment to enable routine studies of impurity transport – multiple injections per discharge (experiments in 2008)
(LaBombard) H-mode Threshold Studies • Physics still uncertain, significant scatter in empirical databases • Role of edge flows in B drift effect opens new avenue to explore • High Priority Experiment: Low density threshold for L-H transition (in baseline scenarios area) • High Priority Experiment: Study slow evolution with improved diagnostics • Especially Er and Ti evolution • High Priority Experiment: Relationship of pressure gradient, collisionality and SOL flows in L-H transition
L-H Threshold: Recent Experiments Found “Two-stage” Transition • Te pedestal begins to develop before L-H transition • Two stages clearly defined in fluctuations • Evolution of Er? (new diagnostics in place) (Hubbard)
Pedestal/Edge Barrier Structure • Issue: predicting width: Concentrate on role of magnetic shear and collisionality • Shear-related quantities (q, d) are the only ones that effect pedestal width in C-Mod • High Priority Experiment: Role of magnetic shear via scans of q, d, k • High Priority Experiment:Separate magnetic shear and plasma flow effects in SOL transport via inner gap scan (Hughes)
Pedestal: Ion Physics • Spectroscopic diagnostics beginning to bear fruit… • High Priority Experiment: Ion channel: measurements of Ti, V, Er in pedestal • Previously mentioned n* scan (Rowan, McDermott) (Marr)
Pedestal Relaxation Mechanisms • ELMy regimes may become more important as we move to lower collisionality with cryopump • ELM research (discussed by others) • Work on QC mode will continue • We’ve observed interaction of QC mode structure and X-point location – needs detailed comparison with code (BOUT) (Lin) PC picks up fluctuations in plasma edge (top and bottom) which are reduced when observation chord is near separatrix
(Zhurovich) non-ITB ITB ITB: Barrier Formation And Control In C-Mod Understood As Interplay Of Density And Temperature Gradients • ITBs created with off-axis ICRH • Physics scenario supported by experiments and simulations. • ITBs In C-Mod Not Dominated by ExB Stabilization • Formation driven by reduction in LT • ITB forms when region of ITG stability reaches (future) barrier foot • Feedback via Ln ITG(+), TEM(-)
Heat pulse slows as it propagates through the barrier ITB Program • High Priority Expt: Verify model for barrier control via TEM turbulence using upgraded PCI measurements • Barrier foot is a particularly interesting region • High Priority Experiment: Measure fluctuations at foot of barrier • Reflectometer • Correlation length measurements • 140GHz channel = 2.4x1020 • Improved Ti profiles with HIREX III • Background Experiments: Prepare ground for barrier experiments w/ modified shear • (Wukitch)
Transport - Highlights • Opportunities to exploit this campaign • Facility upgrades: Cryopump and LHCD will allow important parameter variation (n*, S) • Continuing upgrades in core profile and fluctuation measurements • Enhancements to local computing cluster • Areas of key contribution • Direct manipulation of magnetic shear • Control of collisionality • Self-generated rotation and momentum transport • L/H transition physics: especially flows, B effect • Parameter extension relative to low field tokamak (for example in pedestal or ELM studies) • Reactor relevant ITB regimes